THE HYPERFINE STRUCTURE OF THE 3P3/2 STATE OF NA-23

[1] BLATT JM, 1952, THEORETICAL NUCLEAR

[2] BROSSEL J, 1949, CR HEBD ACAD SCI, V229, P1213

[3] A NEW DOUBLE RESONANCE - METHOD FOR INVESTIGATING ATOMIC ENERGY LEVELS - APPLICATION TO HG P-3(1) [J]. PHYSICAL REVIEW, 1952, 86 (03): : 308 - 316

[4] CASIMIR HBG, 1936, INTERACTION ATOMIC N, P54

[5] CONDON EU, 1951, THEORY ATOMIC SPECTR, P263

[6] DAVIS, 1949, PHYS REV, V76, P1076

[7] Nuclear magnetic moments from the polarization of resonance radiation sodium, 3(2)S(1/2)-4(2)P(3/2), (1/2) [J]. PHYSICAL REVIEW, 1934, 46 (07): : 0583 - 0589

[8] Nuclear magnetic moments [J]. PHYSICAL REVIEW, 1933, 43 (08): : 0636 - 0639

[9] Note on the calculation of zero order eigenfunctions [J]. PHYSICAL REVIEW, 1931, 38 (02): : 248 - 254

[10] An application of the correspondence principle to the question of the polarisation of the fluorescent light [J]. ZEITSCHRIFT FUR PHYSIK, 1925, 31 : 617 - 626

[1] BLATT JM, 1952, THEORETICAL NUCLEAR

[2] BROSSEL J, 1949, CR HEBD ACAD SCI, V229, P1213

[3] A NEW DOUBLE RESONANCE - METHOD FOR INVESTIGATING ATOMIC ENERGY LEVELS - APPLICATION TO HG P-3(1) [J]. PHYSICAL REVIEW, 1952, 86 (03): : 308 - 316

[4] CASIMIR HBG, 1936, INTERACTION ATOMIC N, P54

[5] CONDON EU, 1951, THEORY ATOMIC SPECTR, P263

[6] DAVIS, 1949, PHYS REV, V76, P1076

[7] Nuclear magnetic moments from the polarization of resonance radiation sodium, 3(2)S(1/2)-4(2)P(3/2), (1/2) [J]. PHYSICAL REVIEW, 1934, 46 (07): : 0583 - 0589

[8] Nuclear magnetic moments [J]. PHYSICAL REVIEW, 1933, 43 (08): : 0636 - 0639

[9] Note on the calculation of zero order eigenfunctions [J]. PHYSICAL REVIEW, 1931, 38 (02): : 248 - 254

[10] An application of the correspondence principle to the question of the polarisation of the fluorescent light [J]. ZEITSCHRIFT FUR PHYSIK, 1925, 31 : 617 - 626